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DOI: 10.1002/asia.201201089

Facile Synthesis and Photophysical Properties of Sphere–Square Shape

Amphiphiles Based on Porphyrin–[60]Fullerene Conjugates

Chien-Lung Wang,*

[a, b]

Wen-Bin Zhang,

[a]

Xinfei Yu,

[a]

Kan Yue,

[a]

Hao-Jun Sun,

[a]

Chih-Hao Hsu,

[a]

Chain-Shu Hsu,

[b]

Jojo Joseph,

[c]

David A. Modarelli,*

[c]

and

Stephen Z. D. Cheng*

[a]

Introduction

Driven by noncovalent interactions, self-assembling

process-es are recognized as one of the most important ways to

build up complex supramolecular entities.

[1–7]

Based on

self-assembly principles, various complex functional

supramolec-ular materials have been developed.

[8–14]

The synergy

be-tween geometric complementarity and noncovalent

interac-tions is the determining factor in the formation of the final

structure. Based on dimensionality and geometry,

nano-building blocks can be generally divided into four

catego-ries: spheres (0D), cylinders (1D), discs (2D), and bulk

com-plex structures (3D). Molecules consisting of geometrically

distinct

subunits

are

thus

known

as

“shape

amphi-philes”.

[15–27]

Because the covalent linkage changes not only

the geometry, but also the symmetry of the molecules, the

molecular shape is also an important factor in tuning the

final self-assembled structures in addition to noncovalent

in-teractions.

Porphyrin (Por) and [60]fullerene (C

60

) are representative

2D and 0D conjugated nanobuilding blocks (Scheme 1).

Al-though the major noncovalent interactions are both p–p

teractions, the shape and geometry define the favorable

in-teraction orientations and the resulting supramolecular

ar-chitectures. The 2D nanobuilding block, Por, prefers to form

columnar phases through directional face-to-face p–p

stack-ing,

[28, 29]

whereas the 0D sphere, C

60

, favors the formation of

a plastic crystal phase with a face-centered cubic unit cell, in

which the p–p interaction is anisotropic.

[30]

Covalently

bound Por and C

60

breaks the centrosymmetry of the

origi-nal nanobuilding blocks and gives a series of intriguing Por–

C

60

shape amphiphilies.

[31–38]

In terms of functionality,

cova-lently bound Por and C

60

forms an electron donor–acceptor

dyad. Unique photophysical properties, such as ultrafast

photoinduced charge separation, long-lived

charge-separa-tion state, ambipolar charge transport, and photovoltaic

ac-tivities, demonstrated the potential of C

60

–Por shape

amphi-philes in optoelectronic applications.

[34, 36, 37, 39–43]

Abstract: Molecules constructed from

a

combination

of

zero-dimensional

([60]fullerene (C

60

)) and

two-dimen-sional (porphyrin (Por)) nanobuilding

blocks represent an intriguing category

of sphere–square “shape amphiphiles”.

These

sphere–square

shape

amphi-philes possess interesting

optoelectron-ic properties. To effoptoelectron-iciently synthesize

a large variety of C

60

–Por shape

amphi-philes, a facile route based on Steglich

esterification was developed. The

syn-thetic strategy enables the preparation

of hydroxy-functionalized Por

precur-sors (9–12) with high purity in a

one-pot procedure. All of the C

60

–Por

shape amphiphiles (1–5) can be readily

synthesized in good yields through

sub-sequent

Steglich

esterification

with

a highly soluble carboxylic acid

deriva-tive of methanofullerene (13).

Photo-physical studies indicated weak

elec-tronic coupling between the C

60

and

Por moieties and suggest an

edge-to-face alignment for the moieties. The

fluorescence of electronically excited

Por portions of each amphiphile was

efficiently quenched, which was

indica-tive of electron transfer from

1

Por to

the

C

60

group(s).

Increasing

the

number of C

60

groups on the shape

am-phiphiles led to more pronounced

quenching of the Por fluorescence,

which indicated the potential for more

effective generation of

charge-separat-ed species, C

60



CPor

+

C, from the

photo-excited C

60

–Por shape amphiphiles.

Keywords: fullerenes ·

photophy-sics · porphyrinoids · shape

amphi-philes

[a] Prof. C.-L. Wang, W.-B. Zhang, X. Yu, K. Yue, H.-J. Sun, C.-H. Hsu, Prof. S. Z. D. Cheng

Department of Polymer Science

College of Polymer Science and Polymer Engineering The University of Akron, Akron, Ohio 44325 (USA) E-mail: [email protected]

[b] Prof. C.-L. Wang, Prof. C.-S. Hsu

Department of Applied Chemistry, National Chiao Tung University 1001 Ta Hsueh Road, Hsinchu 30010 (Taiwan)

E-mail: [email protected] [c] J. Joseph, Prof. D. A. Modarelli

Department of Chemistry and The Center for Laser and Optical Spectroscopy, Knight Chemical Laboratory The University of Akron, Akron, Ohio 44325-3601 (USA) E-mail: [email protected]

Supporting information for this article is available on the WWW under http://dx.doi.org/10.1002/asia.201201089.

(2)

Recently, we reported our efforts toward self-assembled,

hierarchical “double cable” supramolecular structures in the

bulk through the design and synthesis of Por–C

60

shape

am-phiphiles.

[44–46]

These shape amphiphiles first form

hierarchi-cal “double cable” columns and further organize into 3D

or-thorhombic or hexagonal columnar lattices.

[45, 46]

An

alternat-ing arrangement of Por and C

60

in a triclinic lattice formed

by trans-diC

60

–Zn

II

Por was also observed.

[44]

These studies

demonstrated an abundance of supramolecular entities

formed by C

60

–Por shape

am-phiphiles and their potential

use in optoelectronic

applica-tions. Because an efficient and

precise synthesis is a

prerequi-site in the study of structure–

property relationships, our

at-tention focused on extending

the previously reported

two-step esterification strategy to

the synthesis of a library of

C

60

–Por shape amphiphiles for

a systematic study. The

struc-tures are thus constructed with

a single Por core, as shown in

Scheme 1. It is evident that,

not only the chemical

composi-tions (C

60

/Por ratio per

mole-cule), but also the molecular

geometries, can be

systemati-cally varied. Intriguing

optoe-lectronic and self-assembly

be-havior of these molecules is

anticipated.

The

synthesis

of

Por–C

60

conjugates mainly involves two

approaches: 1) condensation of

a C

60

-containing component to

form the Por core;

[47–49]

and

2) attaching C

60

to a preformed

functionalized

Por.

[50]

The

preparation of Pors through

the condensation of aldehyde

and pyrrole is known to give

a mixture of compounds that

are usually difficult to

sepa-rate.

[51, 52]

The synthesis of Por–

C

60

by using the first method is

thus costly. The

post-function-alization method circumvents

the difficulties associated with

Por synthesis and has become

prevalent. However, this

ap-proach is also limited by the

low solubility of both Por and

C

60

and the functional group

tolerance of the coupling

reac-tion when considering the

mul-titude of functional groups in the system. Recently, click

chemistry has been applied to the synthesis of such a

con-struct with a triazole linkage.

[53–57]

Our approach uses a

two-step esterification process and introduces

3,4,5-trisdodecy-loxy benzoate and 3,5-bis(dodecy3,4,5-trisdodecy-loxy)benzyl groups with

long alkyl groups to make both components highly soluble,

thereby facilitating the synthesis and purification of the final

molecule.

(3)

Herein, sequential esterification strategies were used to

effectively generate a library of C

60

–Por shape amphiphiles.

First, 5,10,15,20-tetra(p-hydroxyphenyl)porphyrin (6) was

chosen as the core unit and Steglich esterification was used

to sequentially connect the peripheral substituents, which

were 3,4,5-trisdodecyloxybenzoic acid (7) and a carboxylic

acid derivative of methanofullerene (13).

[58]

By taking

ad-vantage of the large polarity difference between the hydroxy

group and the ester group, all of the specifically

hydroxy-functionalized porphyrins (OH-Pors in Scheme 2) can be

prepared effectively and separated easily in a one-pot

reac-tion. The C

60

–Por shape amphiphiles were then synthesized

by treating the OH-Pors with 13 through a second Steglich

esterification. This synthetic procedure has the following

ad-vantages: First, control of the number of functional groups

per Por is achieved at an early stage of the synthesis. As

shown in Scheme 3, monoOH-Por (9), 5,15-diOH-Por (10),

5,10-diOH-Por (11), and 5,10,15-triOH-Por (12) were

sepa-rated and obtained during the first step of the synthesis.

Second, the carboxylic acid derivative of methanofullerene,

which is more time-consuming and costly to prepare, is only

used in the last step of the synthesis. Third, the mild reaction

conditions of Steglich

esterifi-cation prevent potential

de-composition in the reaction to

the conjugated molecules.

Results and Discussion

Synthesis and Characterization

of the OH-Por Precursors

The synthesis of the OH-Pors

is outlined in Scheme 3. The

molecules were prepared by treating

5,10,15,20-tetra(p-hy-droxyphenyl)porphyrin with 2.2 equivalents of

3,4,5-trisde-docyloxybenzoic acid. Mixtures of the reference molecule

(8) and compounds 9, 10, 11, and 12 were obtained through

this procedure; these were readily separated by flash

column chromatography on silica gel as a result of the large

polarity differences in 8–12, thus resulting from the different

number and positions of the OH groups (polarity: 8 < 9 <

10 < 11 < 12). The yields of these reactions were 13 (8), 13

(9), 13 (10), 19 (11), and 20 % (12), with a total yield of all

products of about 78 % after purification. The molecular

structures of 8,

[29]

9, 10, 11, and 12 were characterized by

1

H

and

13

C NMR spectroscopy and MALDI-TOF mass

spec-trometry. MALDI-TOF mass spectra clearly confirmed the

structures of 9, diOH-Por, and triOH-Por. The parent-ion

peaks observed at m/z 2648.02, 1991.39, 1991.41, and

1334.43 in Figure S1 in the Supporting Information

corre-spond to the molecular ions [M

+

] of 9, 10, 11, and 12,

re-spectively, and agree well with the calculated molecular

weights of the corresponding molecules. Although the

5,15-and 5,10-isomers of the diOH-substituted compound cannot

be distinguished from their MALDI-TOF mass spectra,

their molecular symmetry is distinctly different and NMR

spectroscopy experiments can readily distinguish between

the two isomers. As shown in Figure 1, the molecular

struc-ture of 10 includes two twofold rotational axes, whereas 11

only has one. The difference in molecular symmetry leads to

different chemical environments for the b protons on the

pyrrole rings and different chemical shifts and splitting

pat-terns in the

1

H NMR spectra. As a result, only one signal

was observed at d = 8.91 ppm for the b protons of 10, but

three signals were observed at d = 8.96, 8.90, and 8.82 ppm

for the b protons of 11 (Figure 1). Thus, from a combination

of molecular characterization techniques, the molecular

identities of 9–12 were established unambiguously.

Synthesis of the C

60

–Por Shape Amphiphiles

As outlined in Scheme 4, the shape amphiphiles,

mono-C

60

Por (1), trans-diC

60

Por (2), cis-diC

60

Por (3), triC

60

Por (4),

and tetraC

60

Por (5) were prepared by treating 9, 10, 11, 12,

and 6 separately with 13 through a second Steglich

esterifi-cation.

Scheme 2. The two-step synthetic route for preparing the C60–Por amphiphiles.

Scheme 3. Synthetic procedure for the preparation of OH-Pors 9–12. Re-agents and conditions: i) 3,4,5-trisdodecyloxybenzoic acid, N,N’-diisopro-pylcarbodiimide (DIPC), 4-(dimethylamino)pyridinium toluene-p-sulfo-nate (DPTS), tetrahydrofuran (THF)/CH2Cl21:2, 25 8C

(4)

The yields of each shape amphiphile after purification

were 71 (1), 63 (2), 83 (3), 73 (4), and 53 % (5).

Compari-sons of the

1

H NMR spectra of 9 and 1 are given in

Fig-ure 2 a and b. After the esterification reaction, the protons

on the p-hydroxyphenyl group of 9 (d = 8.09 and 7.21 ppm)

shifted downfield to d = 8.26 and 7.60 ppm owing to the

res-onance effect of the electron-withdrawing carbonyl group,

and the signals of the protons on the attached C

60

arm

ap-peared at d = 6.68, 6.46, 5.55, 5.37, and 3.94 ppm. In

Fig-ure S2 in the Supporting Information, the signals between

d = 136 and 146 ppm in the

13

C NMR spectrum of 1

(Fig-ure S2 a) were not observed in

the

spectrum

of

9

(Fig-ure S2 b); this clearly indicates

the presence of the sp

2

carbons

of the C

60

unit. These results

evidently imply the formation

of an ester bond between the

OH-Por precursor and 13. The

1

H NMR spectra of 2, 3, 4, and

5 are also shown in Figure 2 c–

f. The signal of the methylene

groups next to the oxygen

atom (OCH

2

) on the

3,4,5-tris(dodecyloxy)benzoate

of

the Ar

1

arm appear at d =

4.15–4.19 ppm. Comparing the

integration of this signal to

those protons belonging to the

C

60

units, it is clear that, as the

number of C

60

units per

mole-cule increases, the integration

of this signal decreases, whereas those signals belonging to

the C

60

arms show increased integration. In addition,

differ-Figure 1. Molecular structures and1H NMR spectra of a) 10 and b) 11.

Scheme 4. Synthetic procedure for the preparation of C60–Por shape

am-phiphiles 1–5. Reagents and conditions: i) 13, DIPC, DPTS, CH2Cl2,

25 8C; ii) 13, DIPC, DPTS, THF/CH2Cl21:2, 25 8C.

(5)

ent molecular symmetries of 2 and 3 affect the signals of the

b protons on the pyrrole rings of the Por core. In the region

between d = 8.8 and 9.0 ppm, the b protons of the more

sym-metrical compound, 2, has two doublet signals, whereas less

symmetrical 3 has two groups of multiple signals. The

MALDI-TOF mass spectra (Figures S3–S6 in the Supporting

Information) have m/z values that closely match the

molec-ular ions [M

+

] of each C

60

–Por shape amphiphile. These

combined results confirmed the success in obtaining the

C

60

–Por shape amphiphiles.

Photophysical Properties of the C

60

–Por Shape

Amphiphiles

The ground-state absorption spectra of the C

60

–Por

amphi-philes (1–5) and reference molecules 8 and 13 were

exam-ined in THF (Figure 3). Comparison of reference

com-pounds 8 and 13 with 1–5 indicate little, if any, ground-state

electronic coupling occurs between the two chromophores.

The absorption spectra of 1–5 are similar to one another

and are characterized by absorptions in the Q-band region

at 515, 550, 590 and 646 nm, and in the more intense Soret

band region at 419 nm. The two higher energy bands at

l

max

=

258 and 326 nm result from the C

60

groups and the

in-tensity of these bands scales linearly with the number of C

60

groups in each dyad.

Electronic coupling between the Por and C

60

moieties in

covalently bound C

60

–Por derivatives typically leads to

a bathochromic shift of the Soret and Q bands of the Por

moiety.

[42, 60]

The degree of the bathochromic shift depends

on the relative spatial orientation of the C

60

and Por

moiet-ies. Guldi et al. showed that C

60

–Por dyads aligned in

face-to-face orientations underwent bathochromic shifts to

a greater extent than edge-to-face aligned C

60

–Por dyads,

most likely because of stronger Por-to-C

60

electronic

cou-pling present in the face-to-face aligned dyad.

[42]

In the case

of 1–5, bathochromic shifts were not observed in either the

Soret or Q-band absorptions, relative to 8. Thus, electronic

coupling between Por and C

60

in 1–5 is weak and the relative

position of Por and C

60

in 1–5 is likely to be close to an

edge-to-face alignment. Considering the fact that the C

60

moieties in 1–5 are connected to the Por core at only one

point (instead of two points in the study by Guldi et al.),

[42]

the C

60

groups in 1–5 are likely to be oriented away from

the Por core; this accounts for the small Por-to-C

60

electron-ic coupling and lack of a bathochromelectron-ic shift in the

absorp-tion bands.

The generation of charge carriers is a critical step in the

photon-to-electron

conversion

process

in

photovoltaic

cells.

[61]

Previous studies have demonstrated the potential of

C

60

–Por dyads in photovoltaic applications,

[36, 37, 45, 46]

in which

the generation of long-lived charge carriers makes these

ma-terials an attractive component in bulk-heterojunction

pho-tovoltaics. Great interest lies in how the variation in the C

60

/

Por ratio affects the photophysical behavior of C

60

–Por

shape amphiphiles. Because quenching of the Por

fluores-cence (FL) in Por-containing donor–acceptor dyads is

a good qualitative indicator of electron transfer, and

there-fore, of the generation of charge carriers,

[39–41, 43, 62]

we

decid-ed to examine the FL spectra of 1–5 (Figure 4). The FL

spectrum of 8 is typical of tetraarylporphyrins, and has

emis-sion bands at l

max

=

653 and 721 nm (Figure 4 a). The FL

spectra of 1–5 displayed emission bands at the same

ener-gies, but with intensities significantly reduced relative to 8.

The FL quantum yields (F

FL

) of each compound were

deter-Figure 3. Normalized absorption spectra of the C60–Por shape

amphi-philes (1–5) and compounds 8 and 13 in THF.

Figure 4. a) The FL spectra of 8 and dyads 1–5 in THF. b) The quantum yields (FFL) are plotted as a function of the number of C60groups.

(6)

mined and are shown graphically in Figure 4 b. Interestingly,

the F

FL

values decrease from 0.15 for 8 to 0.018 for 1 and

to about 0.001 for 5 as the number of C

60

units increases

from one in 1 to four in 5 (Figure 4 b). The difference in F

FL

between 2 and 3 is less pronounced. The significant decrease

in F

FL

in 1–5 as a function of the number of C

60

groups

pres-ent on the shape amphiphiles is consistpres-ent with previous

work,

[39–41, 43, 57]

thus indicating efficient electron or energy

transfer from photoexcited Por to the C

60

group; this

poten-tially leads to charge-separation (Por

+

CC60



C). The specific

regiochemistry of the attachment points in multi-C

60

bearing

Por shape amphiphiles appears to play a less significant role.

These preliminary results suggest the potential use of these

C

60

–Pors amphiphiles as photoinduced charge-generation

materials in the active layer of photovoltaics. We are

cur-rently using transient absorption spectroscopy to determine

charge-separation and recombination rate constants in these

dyads.

Time-correlated single-photon counting (TCSPC)

experi-ments were used to measure the Por excited-state lifetimes

(t) of 1–5 and reference compound 8, and are summarized

in Table 1. Excitation was performed at the Por Q-band

ab-sorption at 560 nm in THF in these experiments, whereas

the Por emission band was monitored at 651 nm. As

expect-ed, the decay of 8 was monoexponential with a lifetime of

10.1 ns; this was consistent with the literature value of 10–

11 ns for similar Pors.

[63]

The decays for dyads 1–5 were

con-siderably shorter than that of 8 and were best fit by using

two- or three-component global analysis (Table 1). The

life-time recorded for 1 is characterized by one longer-lived

component of 2.16 ns comprising 86 % of the decay and

a second, shorter lifetime of 499 ps (9 %). The data for 2

and 3, which have two C

60

groups positioned at either the

5,10- or 5,15-meso positions, show much shorter lifetime

components of 1.16 ns (86 %) and 331 ps (14 %) for 2 and

1.29 ns (81 %), and 427 ps (19 %) for 3. Similar effects were

observed for 4 and 5. From this information and the average

lifetime (t

avg

) data reported in Table 1, it is clear that the

ad-dition of each C

60

group leads to a decrease in the FL

life-time. These results are consistent with the F

FL

data, which

also showed a marked decrease in the F

FL

values with each

additional C

60

group. On the basis of prior photophysical

ex-periments on Por–C

60

dyads in THF,

[43, 64–65]

the decrease in

the t values of 1–5, compared with 8, were attributed to

photoinduced electron transfer. Electron-transfer rate

con-stants, k

ET

, were calculated from the TCSPC data by using

Equation (1):

k

ET

¼ ð1=t

DA

Þð1=t

D

Þ

ð1Þ

in which t

DA

is the lifetime of 1–5 and t

D

represents the

life-time of model porphyrin 8. The k

ET

values shown in Table 1

were calculated by using t

1

(k

ET1

) and t

2

(k

ET2

), whereas

k

ET(avg)

was calculated by using the average FL lifetime. In

the case of 5, the two shorter-lived lifetime components

were used to calculate k

ET1

and k

ET2

. From this data, it is

clear that the addition of each C

60

group results in increases

in k

ET1

and k

ET2

.

Conclusion

An effective two-step sequential esterification strategy was

developed for the preparation of a series of C

60

–Pors shape

amphiphiles.

The

hydroxy-functionalized Por precursors

(9–12)

were

prepared

with

high purity in a one-pot

proce-dure and all of the C

60

–Por

shape amphiphiles (1–5) were

readily synthesized in good

yields in the subsequent

Steg-lich esterification reaction with

13.

Photophysical

studies

showed that the UV/Vis

ab-sorption spectra of the C

60

–Por

shape amphiphiles obeyed the

simple addition of the

absorp-tion of the C

60

nanoparticles

and the Por core. These results implied weak electronic

cou-pling between the C

60

and Por moieties and suggested that

the relative orientation of the two moieties was close to the

edge-to-face alignment. Compared with reference molecule

8, the FL of the Por core in the C

60

–Por shape amphiphiles

was significantly quenched owing to the presence of the

co-valently bonded C

60

units. The FL quenching became even

more pronounced as the number of C

60

units per molecule

increased from one to four. TCSPC experiments also

showed a decrease in t and an increase in k

ET

of the Por

core with the addition of each C

60

group. Photophysical

studies suggested the potential for the effective generation

of charge-separated species, C

60



CPor

+

C, from the

photoexcit-ed C

60

–Por shape amphiphiles. Further investigations are

on-going with regard to phase behavior, phase structures, and

the potential use of the C

60

–Por shape amphiphiles as light

harvesters and charge-carrier generators in optoelectronic

applications.

Table 1. Summary of time-resolved FL data for 8 and the shape amphiphiles 1–5 in THF.[a]

Compounds Fluorescence lifetime kET1 kET2 kET(avg)

t1[ns] t2[ns] t3[ns] tavg[ns][b] ACHTUNGTRENNUNG[s1] ACHTUNGTRENNUNG[s1] ACHTUNGTRENNUNG[s1]

8 10.1 (100 %) 10.1 1 2.16 (71 %) 0.499 (29 %) 2.02 0.36  109 1.91  109 0.40  109 2 1.16 (63 %) 0.331 (37 %) 1.04 0.76  109 2.92  109 0.86  109 3 1.29 (59 %) 0.427 (41 %) 1.13 0.68  109 2.24  109 0.79  109 4 0.769 (61 %) 0.273 (39 %) 0.68 1.20  109 3.56  109 1.38  109 5 1.25 (4.8 %) 0.511 (43 %) 0.109 (51 %) 0.58 1.86  109 9.08  109 1.63  109

[a] An excitation wavelength of lex=560 nm and an emission wavelength of lem=651 nm were used. [b] The

average lifetimes were calculated by using the formula tavg=a1t1+a2t2+a3t3, in which anrepresents the

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Experimental Section

Instrumentation

All1H and 13C NMR spectra were obtained with a Varian Gemini 300

spectrometer at 300 and 75 MHz, respectively. The1H NMR spectra were

referenced to the residual proton impurities in the CDCl3 at d =

7.27 ppm. The 13C NMR spectra were referenced to 13CDCl 3 at d =

77.00 ppm. MALDI-TOF measurements were carried out on a Bruker Ultraflex III TOF instrument (Bruker Daltonics, Inc., Billarica, MA) equipped with a Nd:YAG laser emitting at a wavelength of 355 nm. All spectra were measured in the positive reflector mode. The instrument was calibrated prior to each measurement with external standards, poly(-methyl methacrylate) and polystyrene. Data analysis was carried out by using flexAnalysis software. Absorption spectra were obtained with a Shi-madzu 1601 UV spectrometer. Steady-state FL measurements were per-formed on an ISA Jobin Yvon-SPEX Fluorolog 3-22 fluorometer with dual input and output monochromators. The samples were prepared in approximately micromolar concentrations in THF (Fischer Scientific, HPLC grade). FL spectra were collected as argon-saturated solutions by exciting at the Soret maxima in S/R mode to correct for changes in the lamp output intensity. FL spectra were also corrected for grating and de-tector response and were performed with 2.5 nm excitation and emission slit widths. Quantum yield measurements were made relative to tetraphe-nylporphyrin (FFL=0.11). Time-resolved FL experiments were

per-formed by using the TCSPC technique. The instrument used in this work utilized pulses from a Coherent cavity dumped 702 dye laser pumped by the 527 nm output of a continuous wave (CW) mode-locked Nd:YLF laser. The FL signal was detected at 54.78 with an emission polarizer and depolarizer by using a Hamamatsu R3809U-51 red-sensitive multichannel plate detector (MCP). Data collection and analysis were accomplished with an Edinburgh Instruments data collection system and the PicoQuant FluoFit decay analysis program, respectively. Time resolution on this in-strument was estimated to be about 10 ps after reconvolution. Time-re-solved decays were fit such that values of c2<1.20 were obtained. Error

limits in these measurements were estimated to be 10 %. All TCSPC experiments were run in argon-saturated solutions in THF with optical densities of between 0.10 and 0.15 at the excitation wavelength (Q-band, lex560 nm) and with detection at lex=651 nm.

Materials

Unless otherwise noted, chemicals and solvents were purchased as re-agent grade and used without further purification. CH2Cl2was purchased

from Acros as anhydrous grade. Toluene was dried over CaH2 under

argon and THF was dried over a mixture of sodium/benzophenone under argon. Both solvents were freshly distilled prior to use. 5,10,15,20-Tetra(p-hydroxyphenyl)porphyrin; 3,4,5-trisdodecyloxybenzoic acid; and the carboxylic acid derivative of methanofullerene (13) were prepared according to procedures reported in the literature.[29, 56]The synthesis of

1[46]and an analogue of 2, trans-DiC

60ZnIIPor,[44]were reported in our

previous work. The samples were kept in vacuum before characteriza-tion.

OH-Por Derivatives

3,4,5-Trisdodecyloxybenzoic acid (1.43 g, 2.12 mmol) was dissolved in CH2Cl2 (80 mL) and then slowly added to a solution of

5,10,15,20-tetra(p-hydroxyphenyl)porphyrin (0.80 g, 1.2 mmol), DIPC (318 mg, 2.50 mmol) and DPTS (633 mg, 2.12 mmol) in THF (40 mL) at 0 8C. After addition, the solution was stirred at room temperature for 1 day. The solvent was then removed in vacuo. The residue was dissolved in a mixture of CH2Cl2/hexanes (1:1) and subjected to column

chromatogra-phy (SiO2, hexanes/ethyl acetate (EA) 40:1 (v/v)). The products were

eluted out with a mixture of EA and hexanes with different ratios as shown below. After chromatography, products were reprecipitated from a THF solution with MeOH.

Compound9

Eluted with hexanes/EA = 8:1 (v/v); yield: 422 mg, 13 %; 1H NMR

(300 MHz, CDCl3): d = 8.96 (s, 4 H), 8.93 (s, 4 H), 8.30 (d, J = 8.4 Hz, 6 H), 8.09 (d, J = 8.4 Hz, 2 H), 7.65 (d, J = 8.4 Hz, 6 H), 7.62 (s, 6 H), 7.21 (d, J = 8.4 Hz, 2 H), 4.20–4.13 (m, 18 H), 1.97–1.82 (m, 18 H), 1.58 (br s, 18 H), 1.31 (br s, 144 H), 0.92–0.88 (m, 27 H), 2.75 ppm (s, 2 H); 13C NMR (75 MHz, CDCl3): d = 165.5, 155.8, 153.8, 153.3, 151.2, 143.4, 139.9, 136.0, 135.6, 134.7, 124.2, 120.5, 120.3, 119.4, 119.2, 114.0, 109.0, 73.9, 69.6, 32.2, 32.1, 30.6, 30.0, 30.0, 29.9, 29.8, 29.7, 29.6, 29.6, 26.4, 26.3, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C173H258N4O16 [M]+: 2647.95;

found: 2647.98.

Compound10

Eluted with hexanes/EA = 3:1 (v/v); yield: 308 mg, 13 %; 1H NMR

(300 MHz, CDCl3): d = 8.91 (s, 8 H), 8.28 (d, J = 8.4 Hz, 4 H), 8.07 (d, J = 8.4 Hz, 4 H), 7.62 (d, J = 8.4 Hz, 4 H), 7.61 (s, 4 H), 7.19 (d, J = 8.4 Hz, 4 H), 4.18–4.12 (m, 12 H), 1.94–1.80 (m, 12 H), 1.59 (br s, 12 H), 1.30 (br s, 96 H), 0.90–0.87 ppm (m, 18 H); 13C NMR (75 MHz, CDCl 3): d = 165.7, 155.8, 153.3, 151.1, 143.3, 140.0, 135.9, 135.6, 134.4, 124.1, 120.5, 120.3, 119.0, 113.9, 108.9, 73.9, 69.6, 32.2, 32.1, 30.6, 30.0, 29.9, 29.9, 29.8, 29.7, 29.6, 29.6, 26.4, 26.3, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C130H182N4O12[M] +: 1991.38; found: 1991.39. Compound11

Eluted with hexanes/EA = 3:1 (v/v); yield: 455 mg, 19 %; 1H NMR

(300 MHz, CDCl3): d = 8.96 (s, 2 H), 8.90 (s, 4 H), 8.82 (s, 2 H), 8.28 (d, J = 8.1 Hz, 4 H), 7.98 (d, J = 8.1 Hz, 4 H), 7.66 (s, 4 H), 7.61 (d, J = 8.1 Hz, 4 H), 6.98 (d, J = 8.1 Hz, 4 H), 4.22–4.18 (m, 12 H), 1.99–1.84 (m, 12 H), 1.59 (br s, 12 H), 1.33 (br s, 96 H), 0.94–0.89 ppm (m, 18 H); 13C NMR (75 MHz, CDCl3): d = 165.7, 155.8, 153.3, 151.1, 143.3, 140.0, 135.9, 135.6, 134.4, 124.1, 120.5, 120.3, 119.0, 113.9, 108.9, 74.0, 69.6, 32.2, 32.1, 30.6, 30.0, 29.9, 29.9, 29.8, 29.7, 29.6, 29.6, 26.4, 26.3, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C130H182N4O12 [M]+: 1991.38; found:

1991.41; [M+23]+

: m/z 2014.42.

Compound12

Eluted with hexanes/EA = 2:1 (v/v); yield: 315 mg, 20 %; 1H NMR

(300 MHz, CDCl3): d = 8.90 (s, 4 H), 8.86 (s, 4 H), 8.28 (d, J = 8.4 Hz, 2 H), 8.06–8.02 (m, 6 H), 7.63–7.60 (m, 4 H), 7.18–7.11 (m, 6 H), 4.18–4.11 (m, 6 H), 1.94–1.84 (m, 6 H), 1.56 (br s, 6 H), 1.43–1.30 (m, 48 H), 0.93– 0.88 ppm (m, 9 H); 13C NMR (75 MHz, CDCl 3): d = 165.6, 155.4, 153.1, 150.9, 143.3, 139.9, 135.6, 135.4, 134.5, 123.9, 120.1, 120.0, 119.9, 118.7, 113.6, 108.9, 73.8, 69.5, 32.0, 31.9, 30.4, 29.8, 29.8, 29.7, 29.7, 29.7, 29.6, 29.5, 29.4, 29.4, 29.4, 26.2, 26.1, 22.7, 22.7, 14.1, 14.1 ppm; HRMS (MALDI-TOF): m/z calcd for C87H106N4O8 [M]

+

: 1334.80; found: 1334.43.

C60–Por Shape Amphiphiles

Compound1

Compound 13 (50 mg, 3.8  102mmol), 9 (100 mg, 3.8  102mmol), and

DPTS (11 mg, 3.8  102mmol) were dissolved in CH

2Cl2 (10 mL) and

cooled to 0 8C. DIPC (5.6 mg, 4.5  102mmol) was slowly added into the

solution by using a microsyringe. The solution was stirred at room tem-perature for 1 day. The solvent was then removed in vacuo. The residue was dissolved in hexanes/EA = 20:1 and subjected to column chromatog-raphy (SiO2, hexanes/EA = 20:1 (v/v)) to allow isolation of 1. The

ob-tained dark brown fraction was then concentrated. The product was dis-solved in CH2Cl2 and precipitated in acetone as a dark brown solid

(106 mg, 71 %).1H NMR (300 MHz, CDCl 3): d = 8.96 (s, 4 H), 8.94 (d, J = 5.1 Hz, 2 H), 8.87 (d, J = 5.1 Hz, 2 H), 8.30 (d, J = 8.4 Hz, 6 H), 8.26 (d, J = 8.7 Hz, 2 H), 7.65 (d, J = 8.4 Hz, 6 H), 7.62 (s, 6 H), 7.60 (d, J = 8.4 Hz, 2 H), 6.68 (d, J = 1.8 Hz, 2 H), 6.46 (br s, 1 H), 5.55 (s, 2 H), 5.37 (s, 2 H), 4.19–4.15 (m, 18 H), 3.94 (t, J = 6.6 Hz, 4 H), 1.96–1.71 (m, 22 H), 1.58 (br s, 18 H), 1.30–1.21 (m, 180 H), 0.91–0.83 (m, 33 H),2.78 ppm (s, 2 H); 13C NMR (75 MHz, CDCl 3): d = 165.4, 163.4, 163.2, 160.7, 153.3, 151.3, 150.1, 145.3, 145.1, 144.8, 144.8, 144.7, 143.9, 143.4, 143.1, 143.0, 142.2, 142.0, 141.9, 141.1, 141.0, 140.5, 139.8, 138.9, 136.8, 135.7, 124.2, 120.4, 119.8, 119.6, 119.1, 108.9, 107.5, 101.9, 73.9, 71.3, 69.6, 68.4, 63.1, 32.2, 32.1, 30.6, 30.0, 30.0, 29.9, 29.8, 29.7, 29.6, 29.6, 29.5, 26.4, 26.3, 22.9, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C269H314N4O23 [M]+:

(8)

Compound2

Compound 13 (86 mg, 6.4  102mmol), 10 (58 mg, 2.9  102mmol), and

DPTS (18 mg, 6.1  102mmol) were dissolved in CH

2Cl2 (10 mL) and

cooled to 0 8C. DIPC (9.6 mg, 7.7  102mmol) was slowly added into the

solution by using a microsyringe. The solution was stirred at room tem-perature for 1 day. The solvent was then removed in vacuo. The residue was dissolved in CH2Cl2and subjected to column chromatography (SiO2,

CH2Cl2/THF = 20:1 (v/v)) to allow isolation of 2. The obtained dark

brown fraction was then concentrated. The product was dissolved in CH2Cl2 and precipitated in acetone as a black solid (91 mg, 63 %).

1H NMR (300 MHz, CDCl 3): d = 8.93 (d, J = 4.5 Hz, 4 H), 8.85 (d, J = 4.5 Hz, 4 H), 8.29–8.23 (m, 8 H), 7.66–7.58 (m, 12 H), 6.68 (d, J = 1.8 Hz, 4 H), 6.45 (br s, 2 H), 5.54 (s, 4 H), 5.36 (s, 4 H), 4.18–4.12 (12 H, m), 3.93 (t, J = 6.3 Hz, 8 H), 1.93–1.71 (m, 20 H), 1.58 (br s, 12 H), 1.30–1.21 (m, 168 H), 0.91–0.83 (m, 30 H), 2.82 ppm (s, 2 H); 13C NMR (75 MHz, CDCl3): d = 165.5, 165.4, 163.4, 163.2, 160.7, 153.3, 151.3, 150.1, 145.3, 145.1, 145.1, 145.0, 144.8, 144.7, 144.6, 143.9, 143.3, 143.1, 143.0, 143.0, 142.2, 142.0, 141.9, 141.0, 140.9, 140.5, 139.7, 138.9, 136.8, 135.7, 124.2, 120.4, 119.9, 119.7, 119.2, 108.9, 107.5, 101.9, 73.9, 71.3, 69.5, 68.4, 63.1, 32.2, 32.1, 30.6, 30.0, 30.0, 29.9, 29.8, 29.8, 29.7, 29.6, 29.6, 29.5, 26.4, 26.3, 22.9, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C322H294N4O26

[M]+

: 4632.18; found: 4632.19.

Compound3

Compound 13 (105 mg, 7.8  102mmole), 11 (75 mg, 3.8  102mmol),

and DPTS (18 mg, 6.1  102mmol) were dissolved in CH

2Cl2 (10 mL)

and cooled to 0 8C. DIPC (12 mg, 9.4  102mmol) was slowly added into

the solution by using a microsyringe. The solution was stirred at room temperature for 1 day. The solvent was then removed in vacuo. The resi-due was dissolved in CH2Cl2and subjected to column chromatography

(SiO2, CH2Cl2/THF 20:1 (v/v)) to allow isolation of 3. The obtained dark

brown fraction was then concentrated. The product was dissolved in CH2Cl2 and precipitated in acetone as a black solid (150 mg, 83 %). 1H NMR (300 MHz, CDCl 3): d = 8.93 (m, 4 H), 8.84 (m, 4 H), 8.28 (d, J = 8.4 Hz, 4 H), 8.26 (d, J = 8.4 Hz, 4 H), 7.66–7.57 (m, 12 H), 6.67 (d, J = 1.5 Hz, 4 H), 6.45 (br s, 2 H), 5.53 (s, 4 H), 5.36 (s, 4 H), 4.18–4.12 (12 H, m), 3.93 (t, J = 6.6 Hz, 8 H), 1.93–1.71 (m, 20 H), 1.58 (br s, 12 H), 1.30– 1.21 (m, 168 H), 0.91–0.83 (m, 30 H), 2.82 ppm (s, 2 H); 13C NMR (75 MHz, CDCl3): d = 165.5, 165.4, 163.4, 163.2, 160.8, 153.3, 151.3, 150.1, 145.2, 145.2, 145.1, 145.1, 144.8, 144.7, 144.6, 144.6, 144.6, 143.8, 143.8, 143.4, 143.0, 143.0, 143.0, 142.9, 142.1, 142.0, 141.9, 141.0, 140.9, 140.5, 139.8, 139.7, 138.9, 136.8, 135.7, 124.2, 120.4, 119.9, 119.8, 119.2, 108.9, 107.5, 101.9, 73.9, 71.3, 69.6, 69.5, 68.4, 63.1, 32.2, 32.1, 30.6, 30.0, 29.9, 29.9, 29.7, 29.6, 29.6, 29.5, 26.4, 23.0, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C322H294N4O26[M]+: 4632.18; found: 4632.22.

Compound4

Compound 13 (118 mg, 8.8  102mmole), 12 (38 mg, 2.8  102mmol),

and DPTS (25 mg, 8.5  102mmol) were dissolved in CH

2Cl2 (10 mL)

and cooled to 0 8C. DIPC (13 mg, 1.0  101mmol) was slowly added into

the solution by using a microsyringe. The solution was stirred at room temperature for 1 day. The solvent was then removed in vacuo. The resi-due was dissolved in CH2Cl2and subjected to column chromatography

(SiO2, CH2Cl2/THF = 10:1 (v/v)) to allow isolation of 4. The obtained

dark brown fraction was then concentrated. The product was dissolved in CH2Cl2 and precipitated in acetone as a black solid (114 mg, 73 %).

1H NMR (300 MHz, CDCl 3): d = 8.91 (d, J = 4.8, 2 H), 8.84 (d, J = 4.8, 2 H), 8.81 (s, 4 H), 8.26 (d, J = 8.4, 2 H), 8.23–8.19 (m, 6 H), 7.64 (d, J = 8.4 Hz, 2 H), 7.61ACHTUNGTRENNUNG(s, 2H), 7.58 (d, J= 8.4 Hz, 6 H), 6.66 (d, J =2.1 Hz, 6 H), 6.45 (t, J = 2.1 Hz, 3 H), 5.53 (s, 6 H), 5.34 (s, 6 H), 4.18–4.12 (6 H, m), 3.93 (t, J = 6.6 Hz, 12 H), 1.92–1.75 (m, 18 H), 1.55 (br s, 6 H), 1.42– 1.22 (m, 156 H), 0.91–0.83 (m, 27 H), 2.82 ppm (s, 2 H); 13C NMR (75 MHz, CDCl3): d = 165.5, 163.4, 163.2, 160.8, 153.3, 151.3, 150.1, 145.2, 145.2, 145.1, 145.0, 144.8, 144.7, 144.6, 144.5, 143.8, 143.8, 143.7, 143.0, 143.0, 142.9, 142.9, 142.1, 142.0, 141.9, 141.0, 141.0, 140.5, 139.7, 138.9, 136.8, 135.7, 124.2, 120.4, 119.9, 119.3, 109.0, 107.5, 101.9, 73.9, 71.3, 69.6, 69.4, 68.4, 63.1, 32.2, 32.1, 30.6, 30.0, 30.0, 29.9, 29.8, 29.7, 29.6, 29.6, 29.5,

26.4, 22.9, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C375H275N4O29[M+H]+: 5297.02; found: 5297.04.

Compound5

Compound 13 (120 mg, 9.0  102mmol),

5,10,15,20-tetra(p-hydroxyphe-nyl)porphyrin (14 mg, 2.1  102mmol), and DPTS (24 mg, 8.4 

102mmol) were dissolved in THF/CH

2Cl2(1:2, 12 mL v/v) and cooled to

0 8C. DIPC (14 mg, 1.1  101mmol) was slowly added into the solution

by using a microsyringe. The solution was stirred at room temperature for 2 days. The solvent was then removed in vacuo. The residue was dis-solved in CH2Cl2 and subjected to column chromatography (SiO2,

CH2Cl2/THF = 10:1 (v/v)) to allow isolation of 5. The obtained dark

brown fraction was then concentrated. The product was dissolved in CH2Cl2 and precipitated in acetone as a black solid (71 mg, 53 %). 1H NMR (300 MHz, CDCl 3): d = 8.79 (s, 8 H), 8.18 (d, J = 8.1, 8 H), 7.56 (d, J = 8.1 Hz, 8 H), 6.65 (d, J = 1.5 Hz, 8 H), 6.44 (br s, 4 H), 5.52 (s, 8 H), 5.33 (s, 8 H), 3.92 (t, J = 6.3 Hz, 16 H), 1.78–1.73 (m, 16 H), 1.43 (br s, 16 H), 1.23 (br s, 128 H), 0.858 (t, J = 6.6 Hz, 24 H),2.82 ppm (s, 2 H); 13C NMR (75 MHz, CDCl 3): d = 165.5, 163.4, 163.2, 160.7, 150.1, 145.1, 145.0, 144.9, 144.6, 144.5, 144.4, 144.3, 143.7, 143.6, 142.9, 142.9, 142.8, 142.8, 142.7, 142.0, 141.8, 141.7, 140.9, 140.8, 140.4, 139.6, 138.9, 136.8, 135.7, 119.9, 119.4, 107.5, 101.8, 71.2, 69.4, 68.4, 63.1, 51.3, 32.1, 29.9, 29.9, 29.7, 29.6, 29.5, 26.4, 22.9, 14.4 ppm; HRMS (MALDI-TOF): m/z calcd for C428H255N4O32[M+H]+: 5960.84; found: 5960.93.

Acknowledgements

This work was supported by the National Science Foundation (DMR-0906898, S.Z.D.C. and CHE-0216371, D.A.M.), the Collaborative Center for Polymer Photonics, AFOSR, the Joint-Hope Foundation, and the Na-tional Science Council of Taiwan (NSC100-2221-E-009-152-MY3). We ap-preciate Dr. Xiaopeng Li and Prof. Chrys Wesdemiotis for assistance with the MALDI-TOF mass spectra measurements.

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Received: November 15, 2012 Published online: February 20, 2013

數據

Figure 2. 1 H NMR spectra of a) 9, b) 1, c) 2, d) 3, e) 4, and f) 5.
Figure 4. a) The FL spectra of 8 and dyads 1–5 in THF. b) The quantum yields (F FL ) are plotted as a function of the number of C 60 groups.
Table 1. Summary of time-resolved FL data for 8 and the shape amphiphiles 1–5 in THF. [a]

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